001     187996
005     20250129094341.0
024 7 _ |2 doi
|a 10.1103/PhysRevB.89.115121
024 7 _ |2 ISSN
|a 0163-1829
024 7 _ |2 ISSN
|a 0556-2805
024 7 _ |2 ISSN
|a 1095-3795
024 7 _ |2 ISSN
|a 1098-0121
024 7 _ |2 ISSN
|a 1550-235X
024 7 _ |2 Handle
|a 2128/8411
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|a WOS:000333125500002
037 _ _ |a FZJ-2015-01485
082 _ _ |a 530
100 1 _ |0 P:(DE-HGF)0
|a Alekseev, P. A.
|b 0
|e Corresponding Author
245 _ _ |a Possible undercompensation effect in the Kondo insulator (Yb,Tm)B${}_{12}$J
260 _ _ |a College Park, Md.
|b APS
|c 2014
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520 _ _ |a The effects of Tm substitution on the dynamical magnetic response of Yb1−xTmxB12 (x=0, 0.08, 0.15, and 0.75) and Lu0.92Tm0.08B12 compounds have been studied using time-of-flight inelastic neutron scattering. Major changes were observed in the spectral structure and temperature evolution of the Yb contribution to the inelastic response for a rather low content of magnetic Tm ions. A sizable influence of the RB12 host (YbB12, as compared to LuB12 or pure TmB12) on the crystal-field splitting of the Tm3+ ion is also reported. The results point to a specific effect of impurities carrying a magnetic moment (Tm, as compared to Lu or Zr) in a Kondo insulator, which is thought to reflect the “undercompensation” of Yb magnetic moments, originally Kondo screened in pure YbB12. A parallel is made with the strong effect of Tm substitution on the temperature dependence of the Seebeck coefficient in Yb1−xTmxB12, which was reported previously
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|a Nemkovskiy, Kirill
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700 1 _ |0 P:(DE-HGF)0
|a Mignot, J.-M.
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|a Clementyev, E. S.
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700 1 _ |0 P:(DE-HGF)0
|a Ivanov, A. S.
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700 1 _ |0 P:(DE-HGF)0
|a Rols, S.
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700 1 _ |0 P:(DE-HGF)0
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|t Physical Review B
|v 89
|y 2014
|x 1098-0121
773 _ _ |a 10.1103/PhysRevB.89.115121
|g Vol. 89, no. 11, p. 115121
|0 PERI:(DE-600)2844160-6
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|t Physical review / B
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